|Publication number||US6984978 B2|
|Application number||US 10/073,542|
|Publication date||Jan 10, 2006|
|Filing date||Feb 11, 2002|
|Priority date||Feb 11, 2002|
|Also published as||CA2476243A1, EP1481256A2, US20030151406, WO2003069690A2, WO2003069690A3|
|Publication number||073542, 10073542, US 6984978 B2, US 6984978B2, US-B2-6984978, US6984978 B2, US6984978B2|
|Inventors||Hong Wan, Jay R. Goetz|
|Original Assignee||Honeywell International Inc.|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (8), Referenced by (13), Classifications (14), Legal Events (4)|
|External Links: USPTO, USPTO Assignment, Espacenet|
The invention relates in general to magnetic field sensors and more particularly to integrated magnetic field sensors formed on a single semiconductor die and requiring the use of a magnetic field for functions such as domain setting, calibration, establishing a bias or offset magnetic field, providing a feedback field, determining a sensor transfer characteristic, or other functions requiring a magnetic field.
Extremely small magnetic field sensing devices can be made using strips of a magnetoresistive film of a material such as Permalloy™. The magnetization of the film forms an angle with current flowing in the film and the resistance of the film varies with this angle. When the magnetization of the film is parallel to the current, the resistance is at a maximum, and when it is perpendicular to the current, the resistance has a minimum value.
Magnetic field sensing devices may be used in many applications including, but not limited to, magnetic signal or power isolation, solid state compassing, e.g., in automobiles; current measuring devices; signature detection, e.g., metal detection; and anomaly detection, e.g., position sensing.
Solid state compassing may be used in personal items, for example, in a watch. Position sensing may be used to sense the position of a medical device, such as a catheter within the body of a patient. These and other applications have created requirements for magnetic sensing devices that are of a smaller size and that require less power than the devices of the past.
The present invention also relates to magnetic field sensing devices and to their use in electrical current sensing and measurement applications. Various magnetic field sensing techniques have been used for the measurement of current. Current sensing can be accomplished using Hall Effect transducers. In one arrangement, an electromagnet having a coil that carries the current to be measured produces a magnetic field. A Hall device is used to sense the magnetic field which is proportional to the current. A pole piece may be used to concentrate the magnetic field where the Hall device is located. The Hall device may be designed to provide an analog output or a digital output. In another arrangement, the current to be measured is passed through a coil on a soft iron core having an air gap. A Hall device is placed in the air gap to the sense the magnetic field generated by the current. This technique can be refined by placing a second compensating coil carrying and adjustable and known current on the iron core that opposes the magnetic field created by the current to be measured. The Hall device then senses a condition when the field from the coil carrying the measured current has been nulled by the field from the compensating coil. The number of turns in each of the coils is used to relate the known current to the current to be measured. One disadvantage of the methods just described is that they require that the current measuring arrangement be inserted into the circuit carrying the current to be measured.
Non-contact clamp-on current measuring devices provide a convenient means for measuring DC and AC line current in a current carrying conductor without the need to interrupt the circuit to insert the measuring device. Present methods of non-contact current measurements in conductors often consist of the use of iron or other ferrous types of magnetic materials configured so as to surround or nearly surround a current carrying conductor in a transformer-like configuration. These present methods, sometimes referred to as a “current clamp” or “clamp-on current probe” are widely employed in measuring a.c. currents in wires and other electrical conductors. These devices provide a means of rapidly measuring the AC current by surrounding the conductor with a closed or nearly closed magnetic circuit which is configured as a transformer which is designed for a convenient ratio for measurement to provide, for example, one milliampere per ampere, or one millivolt per ampere. The output of these clamp-on current probes is then read out on a meter or attached via wires to a multimeter. Electronic displays may also be used to display current values. The use of magnetic materials and the need for these materials to surround the current carrying conductor has some disadvantages.
A second common non-contact method of measuring current utilizes the Hall Effect. A Hall element placed in the region of a magnetic field provides an output voltage proportional to the field. One known current transducer uses a Hall-effect device arranged in a gap of a toroidal core. The conductor carrying the current to be monitored is arranged to pass through the toroid. The Hall-effect element measures directly the flux resulting from the introduction of MMF in the toroidal core due to the current in the conductor. Hall element devices are often utilized for both AC and DC non-contact current measurements in wires and other conductors and are available from manufacturers and distributors of AC clamp-on current probes.
Certain current measuring devices that utilize magnetoresistive sensors and require electrical connection into the circuit being measured are also known. For example, in one arrangement a sensor is mounted on one side of a circuit board with permanent magnets mounted on the same side of the circuit board and near opposite edges of the sensor to provide a magnetic field for initial magnetic alignment and biasing of the sensor. A coil which carries the current to be measured is mounted on the other side of the circuit board and opposite the sensor. For low current measuring applications, the coil may be many turns of wire and for high current measuring applications, the coil may consist of a U-shaped heavy conductor with electrical connections made at the ends of the U. In this arrangement, the sensitivity of the current sensor depends on the magnet strength and location. The matching characteristics of the magnets have a great effect on the accuracy and linearity of the current sensor. The inability to attach magnets, for example by gluing, to achieve the same spacing and alignment in devices of this type will also affect the accuracy and linearity of the sensor. Thus, a need exists for a current measuring apparatus that does not require the use of ferrous materials to surround the conductor in which current is being measured or the use of ferrous materials to increase the flux density, and further provides wide flexibility in current measuring ranges.
The present invention solves these and other needs by providing in a first aspect an integrated magnetic field sensing device including at least two magnetoresistive elements which are biased in a first direction by an integral conductor and are sensitive to magnetic field components in a direction perpendicular to the first direction. The sensitivity of the device to a magnetic field is adjustable and is related to the level of the bias current.
In a second aspect, two of the magnetic field sensing devices are mounted in a housing and, in use, the two magnetic field sensing devices are located on either side of and perpendicular to a conductor carrying a current which is to be measured.
A device for sensing magnetic fields in accordance with the principles of the present invention is shown in the drawings and generally designated 10.
A bias field conductor or coil or current strap 30 is connected between pad 32 and pad 34. Conductor 30 is in a spiral form that extends in a clockwise direction from pad 32 to pad 34. Conductor 30 includes segments 36 which pass above magnetoresistive elements 14 and 18, and segment 38 which pass above magnetoresistive elements 16 and 20. A voltage may be applied between pad 32 and pad 34 to provide current 31 in conductor 30. The current in segments 36 of conductor 30 will create a magnetic field or bias field from left to right in elements 14 and 18. The current in segments 38 will create a bias field from left to right in elements 16 and 20.
In use, device 10 will be sensitive to magnetic field components in a direction perpendicular to a bias field or direction of initial magnetization. With reference to
With reference to
When bias field 42 is of sufficient strength, the magnetization of magnetoresistive elements 14, 16, 18, and 20 aligns in the same direction as the bias field. When applied field magnetic components 44 are present, the amount of rotation of magnetization 42 in element 14 to direction 42 a in
The strength of bias field 42 above the level needed to initially align magnetization does effect the sensitivity of device 10 in that with a lower bias field, the sensitivity will be higher, i.e., the field range will be lower than it would be for a higher bias field. Thus, according to the principles of the present invention, the strength of bias field 42 may be operated at various levels in order to adjust the sensitivity or field range of device 10.
Magnetic field sensing devices are used in a variety of applications, including current measuring applications. For example, a conductor that carries the current to be measured may be located so that the current to be measured provides magnetic field components in the direction of magnetic field components 44. The conductor could be formed as an integral part of device 10 or could be separate from device 10. The conductor could be formed into a coil. Another example of a current measuring circuit using magnetic field sensing devices is shown in
where HS is the stray magnetic field in Oersteds (Oe);
Similarly, the magnetic field intensity at sensor B is given by
Assuming a bridge supply voltage 52 of VCC, the voltage output, VAO at 26 a, 28 a of sensor A is given by
V AO =V CC S A H A +V OA
where SA is the sensitivity of sensor A in mV/V/Oe;
Sensitivity, S is given by the expression
is determined by the Permalloy film and a value of about 0.03 is typical;
Assuming SA=SB, then output 68 of amplifier 66 or
where M is an amplification factor related to the amplification of amplifiers 58, 62, and 66.
According to the principles of the present invention, the sensitivity of sensor A and sensor B may be varied by adjustment of current 57 with increasing current reducing the sensitivity.
Now that the basic operation of the current measuring circuit of
The circuit of
Microprocessor 74, associated circuitry and display 76 may be housed in lower portion 82 of apparatus 80 which may be used as a way of holding apparatus 80.
In the circuit of
Microprocessor 74 can be suitably programmed to duty cycle the current to bias conductor or strap 30. Duty cycling provides the benefit that less power is dissipated in device 10. Considerations include that a 5 milliamp (am) per gauss strap requires 250 mA to provide 50 gauss of field strength. The reaction of the magnetoresistive effect is very fast. The bandwidth is typically in the 1 to 5 MHz range. The circuit of
In addition, microprocessor 74 may be suitably programmed to modulate the current in strap 30 for transmission purposes. In this application, a high frequency AC signal imposed on strap 30 will cause the output to generate “sum and difference” signals which can be used in wireless transmission of sensor data, i.e., similar to AM radio modulation. Since these sensors have high bandwidth, signals in the 5 to 10 MHZ range should be achievable. Modulating the strap would allow the system to avoid DC offsets and low frequency noise, by moving the signal to a higher frequency. Demodulation can be done by detecting the “envelope” of the signal, e.g., 50/60 Hz in the case of commercial power line current measurement.
Device 10 has been described using an illustration of a meander or herringbone type of magnetoresistive elements which may provide advantages. For example, the processing of herringbone type sensors is simpler tan that required for certain other types of magnetic field sensors. In addition, the inherent impedance of herringbone sensors is higher which will be an advantage in some applications. An example of a magnetic field sensor that includes such herringbone elements, but does not include other elements of the present invention is the HMC1501 as manufactured by Honeywell International. However, the principles of the present invention also apply to magnetoresistive elements of other types. For example, the invention applies to magnetoresistive elements which are formed of elongated strips of Permalloy having a pattern of metal overlaid on the strips to form shorting bars. This technique is referred to as “barber pole biasing.”
While device 10 has been described in terms of a four-leg Wheatstone bridge arrangement, it is to be understood that two element bridges utilizing a single current source or utilizing two current sources may be used as well as other alternative arrangements
Thus, since the invention disclosed herein may be embodied in other specific forms without departing from the spirit or general characteristics thereof, some of which forms have been indicated, the embodiments described herein are to be considered in all respects illustrative and not restrictive. The scope of the invention is to be indicated by the appended claims, rather than the foregoing description, and all changes, which come within the meaning and range of equivalency of the claims, are intended to be embraced therein.
|Cited Patent||Filing date||Publication date||Applicant||Title|
|US5825595||May 13, 1997||Oct 20, 1998||International Business Machines Corporation||Spin valve sensor with two spun values separated by an insulated current conductor|
|US5945825||May 15, 1997||Aug 31, 1999||Siemens Aktiengesellschaft||Magnetic field-sensitive sensor device with a plurality of GMR sensor elements which have predetermined directions of magnetization|
|US6020738||May 31, 1996||Feb 1, 2000||Siemens Aktingesellschaft||Device for magnetizing magnetoresistive thin film-sensor elements in a bridge connection|
|US6329818||Jul 14, 1999||Dec 11, 2001||Alps Electric Co., Ltd.||Magnetic field sensor having giant magnetoresistive effect elements, manufacturing method and apparatus therefor|
|US20030057938 *||Aug 26, 2002||Mar 27, 2003||International Rectifier Corporation||Magnetoresistive magnetic field sensors and motor control devices using same|
|DE19743335C1||Sep 30, 1997||Nov 12, 1998||Siemens Ag||Giant magnetoresistive sensor device for external magnetic field detection|
|DE19755673A1||Dec 15, 1997||Jul 1, 1999||Siemens Ag||Magnetoresistive sensor device, especially for non-contact rotary and linear position generator or magnetic field sensor|
|WO1989010570A1||Apr 21, 1989||Nov 2, 1989||Omega Electric Limited||Magnetic field detection system|
|Citing Patent||Filing date||Publication date||Applicant||Title|
|US7250748 *||Oct 1, 2004||Jul 31, 2007||Eaton Corporation||Integrated anti-differential current sensing system|
|US7639006||Jun 2, 2006||Dec 29, 2009||Deffeyes Kenneth S||Detector for magnetic hazards to implanted medical device|
|US8018223||May 23, 2008||Sep 13, 2011||Honeywell International Inc.||Position detection utilizing a rotary array of magnetic sensors with irregular spacing between sensing elements|
|US8519703 *||Mar 20, 2008||Aug 27, 2013||Infineon Technologies Ag||Magnetic sensor device and method of determining resistance values|
|US8717015 *||Feb 12, 2010||May 6, 2014||Robert Bosch Gmbh||Linear-with-magnetic field magnetoresistance device|
|US9104922 *||Nov 12, 2012||Aug 11, 2015||Honeywell International Inc.||Anisotropic magneto-resistance (AMR) gradiometer/magnetometer to read a magnetic track|
|US9207290||Dec 28, 2012||Dec 8, 2015||Industrial Technology Research Institute||Magnetic field sensor for sensing external magnetic field|
|US20050073293 *||Oct 1, 2004||Apr 7, 2005||Hastings Jerome K.||Integrated anti-differential current sensing system|
|US20060276850 *||Jun 2, 2006||Dec 7, 2006||Deffeyes Kenneth S||Detector for Magnetic Hazards to Implanted Medical Device|
|US20080284416 *||May 23, 2008||Nov 20, 2008||Honeywell International||Position detection utilizing a rotary array of magnetic sensors with irregular spacing between sensing elements|
|US20090237075 *||Mar 20, 2008||Sep 24, 2009||Infineon Technologies Ag||Magnetic sensor device and method|
|US20110199078 *||Feb 12, 2010||Aug 18, 2011||Robert Bosch Gmbh||Linear-with-magnetic field magnetoresistance device|
|US20130334311 *||Nov 12, 2012||Dec 19, 2013||Honeywell International Inc.||Anisotropic magneto-resistance (amr) gradiometer/magnetometer to read a magnetic track|
|U.S. Classification||324/252, 324/244|
|International Classification||G01R15/20, H01L43/02, G01R33/09, G01R33/02, H01L43/08|
|Cooperative Classification||G01R33/09, G01R33/096, G01R15/205, G01R15/202|
|European Classification||G01R33/09R, G01R33/09, G01R15/20C|
|Feb 11, 2002||AS||Assignment|
Owner name: HONEYWELL INTERNATIONAL INC., NEW JERSEY
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:WAN, HONG;GOETZ, JAY R.;REEL/FRAME:012593/0829;SIGNING DATES FROM 20020114 TO 20020124
|Jul 20, 2009||REMI||Maintenance fee reminder mailed|
|Jan 10, 2010||LAPS||Lapse for failure to pay maintenance fees|
|Mar 2, 2010||FP||Expired due to failure to pay maintenance fee|
Effective date: 20100110